Method and apparatus for a 3-d electron holographic visual and audio scene propagation in a video or cinematic arena, digitally processed, auto language tracking

ABSTRACT

A system and method for displaying images in three dimensions. The system may include a dual axis four lens system, four LCD switching elements, a pair of LCD switched dual filtered dichroic mirrors, and a pair of half silvered dichroic color filter elements, and two charge coupled device pickups. The system may process light through a number of axis to produce optical disparity for presenting three dimensional video.

RELATED APPLICATIONS

This application is a continuation of co-pending U.S. patent applicationSer. No. 12/931,884, filed Jul. 7, 2010, entitled “METHOD AND APPARATUSFOR 3-D ELECTRON HOLOGRAPHIC VISUAL AND AUDIO SCENE PROPAGATION IN AVIDEO OR CINEMATIC ARENA, DIGITALLY PROCESSED, AUTO LANGUAGE TRACKING,”which is a continuation of now abandoned U.S. patent application Ser.No. 10/958,371, filed Oct. 6, 2004, entitled “METHOD AND APPARATUS FOR3-D ELECTRON HOLOGRAPHIC VISUAL AND AUDIO SCENE PROPAGATION IN A VIDEOOR CINEMATIC ARENA, DIGITALLY PROCESSED, AUTO LANGUAGE TRACKING,” whichare hereby incorporated by reference herein in their entirety.

FIELD OF THE INVENTION

This invention lies in the field of television signal generation andprocessing. More particularly it concerns a system for generating andprocessing TV signals from a visual scene, in which a three dimensionaleffect can be observed in the displayed TV signals, with a mirrored LCDswitched selective color optically oriented digitally controlled lightpath system, and properly oriented optical axes of the three cameratubes or CCD optical pickups, which by digitally or analog modulation,alternately muting the signals from a first, second and third tube orCCD pickups which are adapted to pass the output of the first, second,and third tube or CCD optical pickups which are adapted to pass thefirst, second and/or third primary colors or secondary colors,including:

DESCRIPTION OF THE PRIOR ART

In the moving picture industry, displays of moving pictures have beenprepared and displayed for observation with a three-dimensional effect.This has been accomplished by using two separate cameras, with opticalaxes spaced apart and nominally parallel, but converging at a selectedsmall angle. The light reaching each camera is filtered with one or theother of two primary colors. The corresponding pictures are displayedsequentially, while the observer watches the display with eye glasses,in which one glass passes the first primary color and the second glasspasses the second primary color.

In the moving picture industry to obtain the three dimensional effectrequires essentially doubling the photographic apparatus and doublingthe number of frames of film which are prepared and projected. Thisdoubling of cost has had an affect on the acceptance of the process,which apparently makes the process uneconomical.

Prior art utilized only sequential single muting of one of two selectedprimary colors. This produced excellent dimensionally but destroyedcolor balance. Also, the combination of the 3rd non-switched light beam(green in this example) to the other 2 optical axes caused a shadow ordouble image which the coded glasses could not remove, causing dizzinessand discomfort for the viewer. The new art in this filing ischaracterized in that a primary light beam is passed in conjunction withthe passage of a corresponding secondary light beam thus producingperfect color balance, and removing blurred double imagery, and the needfor coded viewing glasses. In the field of film or television, theapplicants are unaware of any prior art in which a three-dimensionalmoving display does not require special coded glasses to view athree-dimensional effect.

SUMMARY OF THE INVENTION

It is the primary object of this invention to provide a modification ofthe conventional television or film camera system so that a televisionpicture can be generated and processed, such that the display of thatpicture on a television receiver or moving film projection can be viewedin three-dimensional visual display without the aid of encoded glasses.

It is a further object of this invention to provide a method toreproduce or print this process to photographic moving film processdisplays or to static 3-D plate magazine print process.

It is a further object of this invention to provide a modification ofthe television receiver to provide a pseudo three-dimensional display.

It is a still further object of this invention to provide:

1. 3-D Pseudo reformatting formats in tape to tape, film to tape or filmto tape and back to film, for theater release in variable wide screenformats including the following additional feature and formats:

-   -   a. 3-D no glasses display,    -   b. Virtual Vision 3-D CCD LCD glasses display,    -   c. Joy stick zoom and location control,    -   d. High definition (digital line doubling) with wide screen        variable smart reformatting, in variable aspect ratios from 3-4,        9-16, 1-2, and any other aspect ratio configuration as desired,    -   e. 3-D wide digital controlled lens camera with variable aspect        ratio formats additional features as listed in the above        formats,    -   f. A holographic method of digital real-time automatic language        track translation process.

It is the primary object of this invention to provide a modification ofthe TV camera and processing apparatus to make possiblethree-dimensional viewing of the received and displayed signal, whilemaking it possible also to view the display in a conventional manner intwo-dimensional presentation.

These and others objects are realized and the limitations of the priorart are overcome in this invention by utilizing a conventionaltelevision camera, characterized in that an added mirrored LCD switcheddigitally controlled light path system, utilizing corresponding primaryand secondary phased light paths, in which there are three video cameratubes or CCD pickups C1, C2, and C3, receiving light along threedifferent optical axes A1, A2, and A3, which are spaced apart and arenominally parallel to each other in a horizontal plane. Axis A1 isfiltered with filter F1 to pass a first primary color to C1. Similarly,axis A2 is filtered with a filter F2 to pass the camera C2 a secondprimary color, such as green, and the third optical axis A3 is providedwith a filter F3 to pass to the camera C3 the third primary color, suchas blue. The outputs of the three camera tubes or CCDs C1, C2, and C3are processed with video amplifiers V1, V2, and V3 in a conventionalmanner.

A conventional camera control is used which provides a synchronizingbuss that sequences two sub-sweeps, or sub-rasters, which areinterleaved. During a first raster, the output of the first and secondvideo amplifier carrying the red and green signal is muted, or cut off,or disabled and during the second sub-raster the corresponding output ofthe video amplifier V3, carrying the blue signal is cut off or muted.Otherwise the three output signals from the video amplifiers areprocessed in a normal manner to provide a conventional television signalto the transmitter, and eventually to a receiver.

The inventors have discovered that to have a properly color balancedpicture or display, that only complementary primary and secondary colorsshould be alternately switched or muted. In the receiver there will beon a first raster a picture displayed which will be deficient in red andgreen, and on the second raster there will be a picture displayeddeficient in blue and so on When these series of pictures are observedthrough eye glasses (OR NO GLASSES REQUIRED WHEN HOLOGRAPHICALLY MUTEDAS SHOWN IN THE PREFERRED EMBODIMENT) in which one lens is yellow, (thecomplementary or secondary of blue) and one lens is blue (thecomplementary of the secondary color yellow), the display will have athree-dimensional character, dependent on the directions of the opticalaxes of the 1st and 2nd lens.

The principal difference between this invention and the conventionalcamera is, that at least one of the three optical axes representing thethree primary colors must be rotatable toward the other two. Preferablytwo optical axes, the first and third should be rotatable towards thecenter one.

This type of operation can be provided with either one lens, or with twoor three separate lenses. The simplest to conceive of is the one inwhich a separate lens is used in each of the three optical axes. Ofcourse the lenses will be controlled together so that their focus andtheir zoom will be in step with each other, but their optical axes willnot be precisely parallel, as they would be in the conventional camera.

In second embodiment, two lenses can be used. One lens is in the first,or red optical axis. The other is in the third or blue optical axis oneor the other, or both lenses supply the green light to the central orsecond optical axis.

The system can also be used with one lens. In the case of the singlecamera lens, the three optical axes are formed out in front of the linesby use of appropriate mirrors and filters and possible simple lenses.Then the conventional mirrors and filters are used behind the lens andahead of the camera tubes.

A further part of this invention lies in an apparatus modification on atelevision receiver, which is receiving conventional television signalstaken with a single lens, and with the three optical axes preciselyparallel. In this embodiment means are provided for alternately mutingthe red and the green signal from the video amplifiers in the receiver,to the control guns in the tube. If desired one or the other of the redand blue signals can be delayed with respect to the other one, to givethe impression of a three-dimensional viewing situation.

DESCRIPTION OF THE DRAWINGS

THESE AND OTHER OBJECTS AND ADVANTAGES OF THIS INVENTION, AND A BETTERUNDERSTANDING OF THE PRINCIPLES AND DETAILS OF THE INVENTION WILL BEEVIDENT FROM THE FOLLOWING DESCRIPTION, TAKEN IN CONJUNCTION WITH THEAPPENDED DRAWINGS IN WHICH:

FIG. 1 is a schematic block diagram of the modified television camera,adapted to transmit processed primary and secondary color muted signalswhich can be displayed and viewed in three dimensions.

FIGS. 2, 3, and 4 illustrate different embodiments of lenses in order toutilize the three-dimensional display.

FIG. 5 illustrates a detail of the rotation of the optical axes.

FIG. 6 illustrates a further embodiment which invites a modification ofthe television receiver circuit.

FIG. 7 illustrates modified eye glass through which thethree-dimensional picture can be optionally viewed for virtual visionhelmet application.

FIGS. 8-1 to 8-3 illustrates the primary embodiments which utilizes afour lens diachroic filter arrangement digitally switched muting controlof the primary and secondary light beams to achieve dimensionality.

FIG. 8A is a pictorial representation of LCD switching dual mirroredprimary and secondary dichroic filter elements in accordance with anillustrative embodiment.

FIGS. 8B and 8C are pictorial representations of phase switching ormuting patterns in accordance with an illustrative embodiment.

FIG. 8D is a pictorial representation of dimensional viewing based onphase angles in accordance with an illustrative embodiment.

FIG. 8E is a pictorial representation of an embodiment of portions ofthe system of FIG. 8 in accordance with an illustrative embodiment.

FIG. 9 illustrates a top view of a holographic vision hood for 3Dviewing in accordance with an illustrative embodiment.

FIG. 9A illustrates a side view of a holographic vision hood for 3Dviewing in accordance with an illustrative embodiment.

FIG. 10 is a representation of a holographic application for performingtranslations in accordance with an illustrative embodiment.

FIG. 11 is a pictorial representation of a control circuit in accordancewith an illustrative embodiment.

FIG. 12 is a pictorial representation of a circuit for controllingphasing in accordance with an illustrative embodiment.

FIG. 13 is a pictorial representation of a circuit for holographicprocessing in accordance with an illustrative embodiment.

FIGS. 14A and 14B is a pictorial representation of a circuit for stereoholographic output in accordance with an illustrative embodiment.

FIG. 15 is a pictorial representation of sampling clock generators inaccordance with an illustrative embodiment.

FIG. 16 is a pictorial representation of a phasor circuit in accordancewith an illustrative embodiment.

FIG. 17 is a pictorial representation of a phasor circuit in accordancewith an illustrative embodiment.

Referring now to the drawings, and in particular to FIG. 1, there isshown one embodiment of this invention indicated generally by thenumeral 10. This is a schematic block diagram, in which there areseveral parts. The lens and filter portion indicated generally by thenumeral 12, the separate color video camera tubes, indicated generallyby the numeral 14 and the video amplifiers and procession apparatus,indicated generally by the numeral 16.

In the conventional television camera there are three video camera tubesor CCD pickups, each one adapted to pass and process one of the threeprimary colors, such as, for example, red, green and blue. In FIG. 1,the first camera tube or CCD pickup C1, number 42A processed the redlight, camera tube or CCD pickup C2, number 42 B processes the greenlight and the third camera tube C3, 42C processes the blue light. Thelines 18A, 18B and 18C represent the three optical axes. They arenominally parallel, and spaced apart a selected distance. When preciselyparallel to each other, they will not transmit a three-dimensionalsignal. It is only when one or both of the outer optical axes A1 and/orA3 is rotated, so that it intersects the center optical axis A2 at someselected distance in front of the camera, that the appearance of athree-dimensional picture will be evident. The details of rotating theoptical axis will be discussed in connection with FIG. 5.

In FIG. 1 two camera lenses are shown L1, numeral 20A and L3, numeral20C, respectively in the optical axes A1 and A3. The dash lines 22 and24 represent control means, which tie together the two lenses L1 and L3.After that the optical axis moves into the camera by the preciseposition of the video camera tubes can be altered by the use of mirror,etc. However, for convenience and other reasons and without limitationthe three video camera tubes or CCD pickups C1, C2 and C3 will bedescribed as co-axial of the lenses L1 and L3. As the axis A1 is rotatedthe lens and the camera tube will be rotated together, as will bedescribed in connection with FIG. 5. However, by the same means as inFIG. 5, the camera tube can remain stationary while the axis rotates.

Consider the optical axis 18A. Light from a distant scene, off to theleft, arrives at the lens L1 and passes through the lens to beintercepted by partially silvered mirror 28A which passes part of thelight through filter F1, numeral 38A and axis 40A to the camera tube42A. The filter F1 will, for example, be such as to pass only the firstprimary color, red. The output signal of the camera 42A passes by leads43A to the first video amplifier 44A for processing.

Part of the light deflected by mirror 28A passes as beam 30A topartially reflecting mirror 32A. This light is diverted through beam 36,filter F2, numeral 38B and beam 40B, to the second video camera tube orCCD optical pickup 42B. Here the filter F2 is selected to pass thesecond of the primary colors such as green, for example.

Along optical axes 18C light from the scene arrives to the lens 20C andpasses through the lens as beam 26C that passes the light to the filterF3 numeral 38C, beam 40C to the third video camera tube 42C. The filterF3 is designed to pass the third of the primary colors, namely blue, forexample. The output of the video camera C3 goes by leads 43C to thevideo amplifier B3 for processing.

A camera control 58 is provided as is customary in the video camera andno detail of this control is required since the conventional control canbe used. This camera control 58 provides signals to the video amplifiersand to the camera tubes to control the synchronization of that rastersweeps in all of the camera tubes and amplifiers. The camera controlmeans 58 will provide two subscans interlaced, as in the conventional TVsystem. The sync buss 48 is connected also to a flip flop 50 which isresponsive to the synchronizing signal 48 is set to provide a Q′ outputon 52C, during one subraster and a Q output of 52A during the secondraster. On the first subraster the Q output of flip flop 50 via lead 52Acauses (red, for example) video amplifier V1 to pass its output on lead46A to an analog switch 54A. Simultaneously via led 52B the videoamplifier V2 passes its video signal (green, for example) to analogswitch 54B, and the output of the switch 54B goes by lead 46BA to thecamera control. Thus by a combination of the two signals 56A and 46B acorresponding secondary light video signal (yellow, for this example) ispassed to the camera control. When there is a positive signal on lead52A, the analog switch 54A will pass video signals (red for thisexample) on lead 46A to the camera control 58 and simultaneously inexactly the same way via lead 46B the signal foes from video amplifierV2 through analog switch 54B through lead 56B to the camera control 58.On the other hand, when there is no signal on lead 52A, the switches 54Aand 54B will block the transmission of video signals from 46A and 46B tothe camera control.

Similarly when there is a positive signal on lead 52C, the signal fromthe video amplifier 44C, will go by lead 46C to the analog switch 54C,through lead 56C to the camera control. However when a logical zeroappears on the lead 52C, the switch 54C is opened or disabled, and thereis no (blue for this example) video signal output from the videoamplifier 44C to the camera control.

It is therefore clear that the flip flop and the analog switches act asa synchronized switches, and other kinds of switches could be used, so(for this example) that on the first raster the red and green signalsare passed but no blue signal and on the second raster the blue signalis passed, but no red and green signals are passed.

The three video signals on leads 56A, 46B and 56C are then processed in,the camera control to provide the transmitted signal 60 to thetransmitter, and eventually to a television receiver will look like anyconventional picture in three colors and will be two dimensional.However, if as shown in FIG. 7 a pair of eye glasses 97 are provided, inwhich one lens 98A is red passing glass, and the lens 98C in the otherpart of the eye glass 97 is blue passing glass, then the right and lefteye will ultimately see the blue picture and the red picture which arenot precisely aimed at the same scene and therefore will show athree-dimensional optical effect.

The lens and camera portions of the system of FIG. 1 have been repeatedin FIGS. 2, 3, and 4, which show respectively the use of two lenses 20Aand 20C, in FIG. 2 substantially identical to that of FIG. 1. In FIG. 2the axis 18A is shown tilted inwardly in accordance with the dash line18A. The description of FIG. 2 is substantially identical to the portionof FIG. 1 and will not be repeated.

In FIG. 3 the lens and video camera tube and filter portions of thesystem of FIG. 1 are reproduced, except that in FIG. 3 there are nowthree lenses L1, L2 and L3, respectively numbered 20A, 20B and 20C,which define the three optical axes 18A, 18B and 18C. The three lensesL1, L2 and L3 are tied together by controls 22 and 24 as in the case ofFIG. 1, so that they will track each other on focus and zoom. Nointernal mirrors are needed and each lens supplies the light for one ofthe video cameras C1, C2 and C3. The filters F1, F2 and F# are identicalto those in FIG. 1, and the action is substantially as described forFIG. 1. In FIG. 3 the rotation of the two outer axes 18A and 18Cindicates that the two outer axes are rotated inwardly at an angle suchas to intersect the center optical axis 18B at a selected distance infront of the camera. These could be controlled manually as automaticallyor mechanically in response to the focus control 22. This automaticcontrol is shown by the dashed lines 22A, 22B from the control 22 to theoptical axes 18A′ and 18C′. FIG. 4 is another embodiment of the lens andcamera tube section indicated generally by numeral 10B. Here a singlelens L2 is utilized and all of the light going to the three video tubes42A, 42B and 42C are supplied by the single lens L2, by means ofsemi-transparent mirrors, as is done in the conventional video camera.Thus the beam 66B is broken up into two parts 66W which supplies thebeam 70C through filter F3 to the third camera C3. Another part of thelight in beam 66B goes as beam 68B to a second partially reflectingmirror which diverts part of the light as beam 68W to another completelyreflecting mirror and to the filter F1 and to the first video tube C1.Here again the filter F1 passes red light to the video camera tube. Theremaining part of the beam 66B goes as beam 70B to filter F2 whichpasses green light to the second video camera tube 42B.

The main improvement in this embodiment is out in advance of the lenswhere there are three spaced apart filters and spaced apartsubstantially parallel optical axes 18A, 18B and 18C. The filter F11passes red light similarly to FIG. F1 to the lens. Filter F12 passesgreen light and is a substantially identical to filter F2. Filter F13passes blue light similar to that of filter F3. Thus filter F11 is inthe optical axis A1 which passes light of the first primary colorthrough a fully reflecting mirror 64A through a partially reflectingmirror 64B to the lens L2. Similarly the third optical axis 18C passingthrough the filter F13 passes a blue light as beam 66C to fullyreflecting mirror 62C, to partially reflecting mirror 62B, and onthrough to the lens L2 and to the green second camera C2. The greenlight is defined by axis 18B and passes through filter F12 and twopartially reflecting mirrors 62B and 64B through the lens L2 and throughtwo additional partially reflecting mirrors, to the filter F2 and to thesecond video camera tube. It will be clear that a simple lens co-axialwith each of the axes 18A, 18B and 18C preferably in advance of thefilters F11, F12 and F13 may serve to better define the three opticalaxes.

Again, if the axes 18A, 18B and 18C are precisely parallel, there willbe no three-dimensional optical effect; however, if the axis 18A isrotated inwardly as shown by the dash line 18A′ there will be somecontribution to three dimensionality of the display.

One of the problems of rotation of the optical axis in conjunction withthe use of mirrors is important since the light passed through filterF11 must be precisely focused and positioned with the other two lightcomponents, even though the axis 18A is rotated. To do this the axis18A′ is rotated at the center of the mirror 64A as shown.

Referring now to FIG. 5 which is designed around the schematic diagramof FIG. 4, the nominal direction of the optical axis 18A is shown, andthe rotated axis 18A′ is shown. The center of rotation is at the centerof the mirror 28A. In the drawing the element 76 is a stationarycircular concave rack, and 76 is a circular convex rack, which isattached to and moves with the axis 18A as shown by the dashed line 78A.Numeral 8C represents a small pinion positioned between the two racks 76and 78. As the rack 78 moves through a selected angle, say 10 degrees,the pinion 80 will move only half that distance. Thus as the axis 18Arotates to 18A′ the plane 82 of the mirror 28A will rotate to 82″through an angle 21 just one-half of angle 23.

As the axis 18A is rotated, and drives the rack 78 the mirror 28A willfollow in proper angle, so that the entering light through the lens 20Awill be precisely in the same beam 30A, even though the axis doeschange. Thus the picture passed through the beam 30A to the secondcamera tube will not move even though the optical axis changes.

As shown in FIG. 1 green light is supplied to the camera C2 from lensesL1 and L3. While the pictures will be stationary in view of the rotationof the axes 18A and 18C, the pictures that are represented will beslightly different and therefore there may be some minor blurring in theyellow picture in which case one of the other mirrors 28A or 28C can beremoved so that the green light is supplied only by one lens L12 or L3.

In order to utilize the improved camera system of FIGS. 1, 2, 3, and 4,all that is needed to view the reproduced pictures in the receiver isthe eye glass 97 shown and described in FIG. 7. If the glasses of FIG. 7are not used, then the picture produced by the television signals fromFIG. 1 will look like any conventional television signal and will beonly two-dimensional.

Referring now to FIG. 6 there is shown an embodiment in which thetelevision receiver is modified to provide a pseudo three-dimensionalviewing. There will only be a two-dimensional, although there may be apsychological effect suggestive of three dimensionality. The actual TVtransmitted picture, arrives on lead 90 to the TV tube 85 in thereceiver 84 f. This is strictly a two dimensional picture as isconventional. However, what has been done is to take a synchronizingsignal either from the TV circuit on lead 90, or from the local powersystem, 60 cycle power 92, which drives, through lead 92A, a flip flop93. This flip flop through the Q and Q′ outputs, control two analogswitches, 88A and 88C. These switches sequentially control and mute thered signal, and then the blue signal; one in one sub-raster, and theother in the other sub-raster. Thus the video amplifier outputs, on lead89A, the red signal, which goes through the switch 88A to the couplingunit 87, to control the red gun. But the Q and Q′ signals alternatelymute the red and the blue by putting a high signal, or logical one, onthe lead 94A to enable the red signal, or on 94C to enable the bluesignal. If desired 89C (or in lead 89A) an analog phase shift or delayregister 96 can be inserted in the lead so that the display of the bluesignal (or the red signal) will be delayed or phase shifted from thedisplay of the other signal, and will psychologically provide animpression of three-dimensionality.

What has been described is an improvement in video camera and processingapparatus for generating television signals from a visual scene, suchthat these signals when reproduced in a receiver and viewed with coloredglasses will give the impression of three dimensionality, to the picturedisplayed on a two dimensional surface.

While the invention has been described with a certain degree ofparticularity, it is manifest that many changes may be made in thedetails of construction and the arrangement of components. It isunderstood that the invention is not to be limited to the specificembodiments set forth herein by way of exemplifying the invention, butthe invention is to be limited only by the scope of the attached claimor claims, including the full range of equivalency to which each elementor step thereof is entitled.

The Primary Embodiment

In FIGS. 8-1 to 8-3, the accomplishment of a true holographic mutinglens camera system is utilized in this embodiment by implementation ofan adjustable angled and muting switchable dual axis four lens system,L1, L2, L3 and L4, with LCD optical muting S1, S2, S3 and S4 and alsoutilizing the use of two 45 degree angled to the horizontal plane HP1color LCD switched dual filtered dichroic half silvered mirror andmirrored light path systems LD1 and LD2, two forward 45 degrees to thehorizontal plane facing each other half silvered dichroic color filterelements DI1 and DI2, two 45 degree angled to the horizontal plane HP1half silvered mirrors HS5 and HS6, two video pickup tubes or CCD RBGthree color pickups CD1 and CD2, and additional high speed holographicmuting (section B of FIGS. 8-1 to 8-3) before the combined RGB signalsare routed to standard camera control circuitry.

Looking at FIGS. 8-1 to 8-3, a mirrored LCD switched digitallycontrolled light path system, utilizing corresponding primary andsecondary SB2 and SB1 phased light paths, in which there are two fullcolor video camera tubes or CCD pickups CD1 and CD2, receiving lightalong two different optical axes A2 and A3, which are spaced apart andwhich are nominally parallel to each other; and two additional lightpath axes A1 and A4, joined via half silvered mirrors hs1, hs2, hs4 andhs5 to light path axes A2 and A3. A1 and A4 light path axes are minutelyangled SA1 and SA2 to each other in a horizontal plane, to produceoptical disparity for dimension. The angle SA1 and SA2 of the two saidaxes being angle controlled to a small selected angle by 5 worm gearsW1, W2, W3, W4 and W5 with synchronous step motors SM1, SM2, SM3, SM4and SM5. Two of the said worm gears W1 and W2 are used to control thesmall selected angle SA1 and SA2 of the two outside lenses, L1 and L4inwardly toward each other. Two additional worm gear W3 and W4 controlsare used to adjust horizontal positioning of the outside dichroic dualfilter mirror systems LD1 and LD2. The one remaining worm gear W5 isused to adjust the distance DS1 of the center front mirrored 90 degree Vshaped reflecting half silvered internal filter dichroic mirrors DI1 andD12. These digital step controlled worm gears are functionally tied vialead Z1 to the synchronized zoom function control Z2 of the 4 lenses L1,L2, L3, L4 and L5 which are also synchronously focused and aperturecontrolled.

Again looking at FIGS. 8-1 to 8-3: Two mirrored LCD switched digitallycontrolled light path systems, utilizing corresponding primary LB2 andLB3 and secondary SB2 and SB1 phased light paths, in which there are twovideo camera tubes or CCD pickups CD1 and CD2, on axes A2 and A3,receiving light from the two different LCD optically switched S2 and S3muted optical axes A2 and A3, and which are spaced apart and arenominally parallel to each other in a horizontal plane HP1. The saidaxes A2 and A3 additionally utilize light from light path systemsoriginating from axes A1 and A4 as they are filtered and selectivelydigitally switch controlled by LCD optical switches selectively dualfiltered to primary or secondary light beams by dichroic half silveredHS4 and HS3 light path reflecting mirror systems LD1 and LD2, toalternately provide by LCD optical light switch means primary andsecondary light sources which are combined via half silvered mirrorshs1, hs2, hs4 and hs5 with primary light path axes A2 and A3 as light isLCD optical light switch controlled and combined from lenses L2 and L3through dichroic filter elements DI1 and D12, to final read out by CCDRGB optical pickups CD1 and CD2. In FIG. 8A is a detailed look at theLCD Switching Dual Mirrored Primary and Secondary Dichroic FilterElement: a multiple element sandwich consisting of 2 sheets of coatedglass, the first said glass element GL1 with a primary color filter gelcoating F1 on the front and a half silvered mirror coating on the backHS1. The second plane of glass has a primary color filter gel coating F2on the front and a fully silvered mirror coating M1 on the back of thesaid glass.

Sandwiched in between the two said coated pieces of mirrored glass is afull plate LCD optical element switch S1, which when empowered by a plussignal or pulse via lead L1 to the clock enable input of the said LCDS1, momentarily goes full plane opaque or optically transparent for theduration of the pulse width of said flip flop FF1 or digital pulseoutput L1.

When the said LCD light switch S1 is not enabled by said control pulselead L1, the LCD light switch S1 turns off and blocks all light fromgoing through the plane of the said LCD light switch S1. Thus a primarylight beam is reflected back out as same color as the primary gel F1.

Alternately when the said LCD switch S1 is enabled with a positive goingpulse from said lead L1, the LCD optical switch S1 goes opaque allowingthe light beam SL2 to continue through S1 through the gel coating F2,glass plane GL2, to strike the fully silvered mirror coating M1 to fullyreflect outward completely as secondary light beam SL2.

In FIG. 8C is described and illustrated the 4 phase switching or mutingpatterns of Starcam (FIGS. 8-1 to 8-3 herein described as Starcam).Muting of the primary and secondary light beams is shown as they areactivated by the 2 phase control flip flops (FF2 and FF1 of FIGS. 8-1 to8-3). The four phases are shown by column 7, 8, 9, 10. Column 7 revealsthat in phase 1 Starcam admits and processes on axis 1 (A1 of FIGS. 8-1to 8-3) a yellow filtered beam via (LD1 of FIGS. 8-1 to 8-3) andcombines it, via half silvered mirrors HS5, HS1 and HS2 with a bluefiltered light beam from (A3 of FIGS. 8-1 to 8-3) axes 3 through halfsilvered mirror HS6 to the right optical CCD pickup CD2.

Similarly, phase 2 (column 8) shows the green light beam from axis 2 viahalf silvered mirror HS1 and color gel FLG, combined with light fromlens 4, axis 4 (L4 and A4 of FIGS. 8-1 to 8-3) via half silvered mirrorHS3, HS6, HS2 and HS1 to optical RGB CCD pickup CD2 for cameraprocessing.

Phases 3 and 4 similarly emit phased corresponding primary and secondarylight holographic beams for processing to the high speed holographicmuting of FIGS. 8-1 to 8-3 section B to the camera control, according tothe chart as shown in FIG. 8C.

Dual CCD Ultra Vision Hood

In the prior art of hood or helmet viewing of television signals theapparatus is bulky and heavy and apparently expensive to build, and doesnot receive conventional television signals.

Looking at FIG. 9: By utilizing the above described Starcam holographicprocessing of video signals and a new high density light weightstyrofoam casing to house the LCD switching elements 3 and 5, and CCDdisplay elements 2 and 4, and an improved focusing system thatautomatically aligns the viewing area of the CCD display elements 2 and4 when adjusted by one single rocker switch which activates an internalstep motor 9 and worm gear assembly 9 and 6 and bracket 8 to allow theviewer to focus the LCD, CCD elements incorporated with the electronicholographic switching of the dual LCD switches 3 and 5 and dual CCDelements 2 and 4 as shown in the above described Starcam System (FIGS.8-1 to 8-3 section B) allows for normal video signals to be convertedinto a three-dimensional display commonly described as Virtual Vision,allowing 3-D Virtual Vision Viewing of a Visual Scene from eithersignals from the Starcam System or nominal video signals comprising;

Description of the Drawing FIG. 9

The dual CCD Ultra Vision Hood for viewing visual scenes in 3-DHolovision is compatible with the above described primary embodimentStarcam System, of FIGS. 8-1 to 8-3, herein referred to as The StarCamSystem, comprising a light weight styrofoam hood element FIG. 9 and FIG.9A that is horizontally cut into two sections (1 a and 1 b of FIG. 9A)that can be separated (2 of FIG. 9A) for component insertion of the twoCCD display devices 2 and 4 each positioned behind LCD digitallyswitched LCD optical switches 3 and 5, that when focused by a motordriven worm gear 6 attached to bracket 8 enables the CCD LCD assembly 2and 3, 4 and 5 to adjust to viewer's eyes precisely at a correct angle20 and distance and distance 21 and 22 required for a three-dimensionalperception of a video scene when switched sequential in phase with anelectron hologram signals (FIGS. 8-1 to 8-3, section B) generated as isthe Starcam Camera System above described.

Also provided are video amplifiers 6 and 7 required by the two CCD-LCDdisplay units shown inserted on either side of hood element.

Inserted in the front of hood element 1B is provided a wide angle lensand video camera system 10 which optionally may be turned on for viewingoutside the hood area without removing the hood FIG. 9A element from theviewer's head.

Formed outside of the styrofoam hood element is provided an indenture 11for a stereophonic audio headset of conventional head phones forreceiving audio signals from the video source displayed by the CCDdisplay elements 2 and 4 and LCD optical switches 3 and 5 inside thehood element. The audio amplifier 14 and FM receiver 13A is insertedoutside the hood element in the rear behind the head hole 13 of the hoodelement 1B.

The power supply consists of 8 rechargeable batteries placed into 8holes in the styrofoam mold situated in back behind the molded head hole13. Replacement is accomplished by separating the hood element 1 a and 1b of FIG. 9A.

A control panel 7 a coordinates all the electronics of the dual CCD LCDhood system is located on the right front right side of the hood elementindented into the styrofoam and includes rocker switch 15 for focusingthe viewing of CCD-LCD viewing elements, positioned for ease of controlof the viewer. The front slots 16, 17, 18 and 19 indented in thestyrofoam casing 1 b of the hood element 1 b contain video processingelectronics for processing nominal two-dimensional video signals intophased three-dimensional signals as described in the above shown StarcamHolographic Video System. (FIGS. 8-1 to 8-3, section B)

By utilizing the dual CCD-LCD elements of the Ultra Vision Hood SystemFIG. 9A coupled with the holographic muting system as described in FIGS.8-1 to 8-3 section B of the Starcam System, a holographic Visual Sceneis displayed from video signals transmitted (TR1 of FIGS. 8-1 to 8-3)from the Starcam System.

For pseudo dimensional processing and display of two-dimensional videosignals to 3-D holographic visual displays, a composite video signal maybe imputed at VII of FIGS. 8-1 to 8-3 into the video processor V12 whichoutputs separate RGB signals into the holographic processor circuitryshown in section B of FIGS. 8-1 to 8-3, for 3-D holographic conversionfor viewing in three-dimensions, and sequentially transmitted to thetelevision receiver 13 a, or by direct cable, or infrared roomtransmission of the video signal to the Ultra Vision Hood for signalprocessing and display of a visual scene in 3-D holography.

Looking at FIG. 8D: The inventors have theoretically discovered thatlight photons have a left and right spin according to whether the lightbeams are coming in from left viewpoint perspective or a right viewpointperspective, and that although the speed of light particles is constantthe speed of said photo spin determines phase angle and color of lightin dimensional perspective, and determines the perspective and distanceof a particular imagery source. If the perspective is dead center thenthe phase angle of the photon is 0 degrees. If the perspective angle iscoming from the right the spin of the photons will be clockwise. If theperspective is to left of a perpendicular line the phase spin of thephoton will spin opposite. The point of focus and perspective willdetermine the phase angle and spin of the photon. From a reference ofperpendicular line to the horizontal plane, a 90 degree line from theaxis of perspective drawn from perspective point will indicate phase ofthe proton, and will reflect focus and depth of field. It is thereforepossible to reproduce, by the Starcam circuitry exact phasings, fordimensional perspective of a reflected light path visual scene, makingit possible to generate real time or pseudo 3-D reproduction of a visualscene.

It is also shown by the inventors that the selected color phasings ofthe Starcam circuitry can reproduce perspective and dimensional depth offield.

As indicated by the drawing, the four lenses of Starcam each generate aparticularly different phase relationship to the visual scene beingphotographed holographically. These phases are directly tied to thedistance focusing and holographic perspective of the Starcam cameralenses.

In column “A” is shown examples of the holographic three-dimensionalphasings and digital duty cycles generated by lenses at differentoptical axis angles on a horizontal plane when focus is set FC1 atnominally 50 feet. Lens one L1 will generate a digital duty cyclephasing as depicted in duty cycle A1. Assuming that this is the dutycycle of the output of a control flip flop which mutes the RGB ofStarCam, a very small duty cycle for the red signal would limit the timefor the transmission of the red signal while green would enjoy aconsiderably larger potion of the duty cycle timing of the said flipflop control signal. Lens L2 90 degrees to a horizontal plane axisdemonstrates a perfectly square duty cycle. Thus the red and greenmuting cycles would perfectly equal. Lens L3 indicates a widening of theduty cycle of the said control flip flop. Lens L4 indicates even a moreextreme unbalance of the duty cycle. Also note the slightly differentphasings of perspective point B with focus set at 20 feet (f2 and FC2).

Variable high speed scanning of the primary and secondary combinationcolor muting with selected phasings allows for the video pickup tubes orCCD pickup elements to show alternate and variously selected phases ofdepth of field focusing for three-dimensional imagery.

The following sub-atomic phasings are utilized to clock the high speedRGB switched phasings of the StarCam system as shown in FIGS. 8-1 to 8-3section B, imputed at SA1 in FIGS. 8-1 to 8-3.

This is a holographic control pulse generating system for processingtelevision signals form sub-atomic phasing in which a high definitiondimensional effect can be observed in the displayed television signals,by providing photon phasings that are holographically orientated andsub-atomically controlled by electron mueon phasings which when mergedwith conventional television signals phase the normal television signalsinto a holographic display on the standard CRT, which produces adimensional visual scene from a conventional or standard televisioncamera, or video signal.

The displayed visual scene, when viewed on a standard televisionreceiver, is perceived as a 3-dimensional image with an expanded depthof field viewed in a high definition format.

Phasings of the W and Z particles of the electro Weak Force asestablished by Cola Rubia and his colleagues at Cern in 1983 can bereplicated electronically by certain holographic electronic phasing,which can be used to create high definition 3-D TV.

Electronic Sub-Atomic muting or Mueon electron Phasing is accomplishedsimilarly to sustain the same sub-atomic Mueon electronic results asshown in the Cern Experiment by Cola Rubia and his colleagues which wasset up to prove the existence of the W and Z phasing of the Electro WeakForce, i.e. sub-atomic proton and anti-proton particles were phased inopposite direction in the Cern Cyclotron and photographed at a collisionpoint to show the existence of separate Mueon tracks phased differentlyproving the existence of the mueon electron particles W and Z. The Wenergetic particle providing a single straight track proving itsexistence, and the Z energetic particles providing two straight tracksof electron Mueons, to prove its existence.

The electronic television camera as we know today collects visual data(Photons) on to photo sensitive material (phosphorus) which is scannedhorizontally synchronously line by line and reproduced to a televisionmonitor (CRT), in which the series of line scans are reproducedfaithfully to a CRT or phosphorous screen which lights up dot by dot,line by line. The phosphorous in the vacuum tube presents or replicatesthe visual scene focused on by the lenses of the electron TV camera.

In today's TV system a two-dimensional scan is shown or visualized tothe flat TV surface or CRT. What is now shown and described is (insteadof a two-dimensional flat image) an image produced to the CRT by asub-atomically phased electronic pattern which produces the same imageto the CRT but transformed into a sub-atomically phased holographicimage. The CRT's phosphorous dot pattern is sub-atomically phasedagainst each other and produces a third image or hologram which whenviewed by the human visual system is visualized in the brain as a3-dimensional holographic image, processed into a magnetic sub-atomichologram, which is magnetically scanned from both left and right brainsinto a high definition visual image.

What is being shown and characterized is an electronic phasing circuitthat emulates holographic phasings of sub-atomic structure that sustainselectronic phasings of the W and Z Mueon energetic mueon electrons,allowing continual use and control of sub-atomic phasings, to encodeholographically the electron Weak Force which in turn controls theStrong Electrical Magnetic Force, which in turn may be used to encodehigh definition dimensioned signals to a CRT.

Instead of using Mega Volt high cost cyclotrons to smash by brute forcesub-atomic particles with billions of volts to produce sub-atomic mueonelectron phasing that last only billionths of a second we electronicallyachieve holographically control of the phase of the sub-atomic weakforce to in turn sustain indefinite control of the Electro-MagneticStrong Force, and the Sub-Atomic Strong Force. (The electro Weak Forceacting holographically as the control factor over the Electro-MagneticStrong Force and other forces.)

Thus, we contend that such holographically phased Sub-Atomic patterns (W& Z) exist in matter, or nature (not just as results of a smashed atomor protons) but as holographic sub-atomic control phasings, which inturn determine the very structure of (atomic) matter existing as the DNAof matter, (MDNA) cracking the door to a new form of sub-atomicalchemistry.

Thus, a key to understanding ordinary matter is shown utilizingholographic electronic phasings to control the Electro Magnetic Force,Gravity, Strong Force, and the Electro Weak Force.

As any molecular structure or matter is spun horizontally, naturalmagnetic poles are created vertically at the center of the spin. (i.e.gravity)

The angle of the poles [Vp(x)4] determines phase angle of the spin inrelation to other spinning bodies of matter (as in magnetic masses ofphotons) in proximity to each other. A spinning object spinning atspecific rates different to an object in proximity would be out of phasewith each other. (i.e., if they were spinning at the same rate(regardless of size or weight) they would be in phase with each other.)

Thus, strings of photons can attach to each other and produce the samecolor balances. Photons out of phase would produce other colors, etc. Asan example: as in photon molecular structure, galaxies, indeed the wholeuniverse, when spinning a center of gravity is created or installed. Thenuclei of atoms, the center of the Sun, the center of galaxies, theuniverse, even photons spin. (i.e., left handed or right handed; ref:Scientific American “Photons have a right handed or left handed spin”,and their poles would have a different angle, in relation to otherbodies around them.)

The angle of the poles Vp(x)4 determines phase or angle of the spin inrelation to the spinning bodies of matter in proximity with each other.Spinning objects spin at specific rates different to objects inproximity with each other would be out of phase. If they were spinningat the same rate and coming in from the same angle of sight (regardlessof size or weight), they would be in phase with each other. Thus stringsof photons, at a particular angle, can attach to each other and producethe same ratio of color balances per angle and distance. Photons out ofphase, coming in from a different angle and/or distance, would produceslightly different hues and colors, producing dimensional phase angles.(i.e., dimensional weight.)

We can now postulate that all matter has a center of gravity as producedby its spin rate. (i.e., nuclei of every atom.) If they were spinning atthe same rate (regardless of size or weight), they would be in phasewith each other. Thus strings of photons attached to each other andproducing the same color balances, would indicate origin of the sameangle and distance. Photons out of phase would produce slightlydifferent hues of color, indicating origin of a different angle and/ordistance.

We can also postulate that any visual scene of matter has a center ofgravity as produced by its phased spin rate of the combinedholographically phased nuclei of all the atoms, thus giving the humanbrain critical information to decipher dimensional information regardingdepth, angle, perspective, and even related hue color information. As anexample, the so called “red shift” which scientists utilize to measurethe distance to distant star systems, is a prime example of colorfrequency phase shifting information provided by incoming spinningphotons to give super accuracy concerning distance and angleinformation, showing that photons can be affected by time and spacegravity continuums.

Whether of photons or atoms, etc. rate of spin determines the force andphase of the mass of the object. (i.e., gravity intensity of the core ornuclei Sr(x={G(x)2] when G=[Sr(prp)2]. Even photons have a g(x)2 core,and resulting vertical poles.)

Simply by changing phasing of the sub-atomic photon particlesholographically, to new phase counts, you can position an imageholographically on the electronic CRT, producing dimensional weight.

Nature postulates that all matter has a center of gravity as produced byits spin rate, (i.e., nuclei of every atom and its associated group ofcontrol electrons.) By phase manipulation we can offset the center ofgravity (dimensional weight) of a group of photons causing thereplication of dimensionary information coming to the eyes and thebrain. Via its method of scanning horizontally. The rods and cones ofthe human eyes, dimensional phase information is transmitted to thebrain. Histeresis Sub-Atomic-Mueon holographic phasings replicate to thebrain's sensors visual scenes dimensionality, via sub-atomic phasedelectron mueon brain holograms.

Holograms are known and visualized in nature, such as rainbows, layeredfrost on a window, or they can be produced with split laser beams ofcoherent light; or magnetically produced as in seismographic equipment,as described by Dan Silverman in his patents; or as in our description,they can be produced as sub-atomic patterns phased against each other,coherently, on a CRT or television monitor.

The di-fraction of light as provided by a triangular prism piece ofglass to produce a rainbow spectrum pattern order of color is anotherprime evidence of the phasing of the spinning photons encoding color, asrelated to incoming angle, (dimensional weight) distance and spin phaseof the incoming photons. As you go from one end of the spectrum of therainbow color encoding, the lower frequency colors spin slower than thehigher frequency brighter colors. Their spin phase rate (dimensionalweight) is ordered exponentially according to their perspective color.

As in a prism, where colors separate out at different successive angles,closely phased strings of photons merge together because of theirrelative mass and spin rates. As they beat against each other, withconstructive and destructive muting, holographic nodes appear. Finallyas individual photons phase together they lock harmonically intosuccessive different nodes of primary and secondary order, mimicing the(hex) hexagonal order and structure of photons. (i.e., three primarycolors red, blue and green, and secondary phased color masses ofmagenta, cyan and yellow.)

Sub-atomic muezzin energetic electron phasing is the heart of thisdescription or invention, and presents a new form of holography, indeeda new form of controlling and understanding the visual format of thehuman brain in visualizing dimension in nature.

By controlling the spin rate and phase rate [Sr(x)2, and Pr(x)4], and bycontrolling the spin rate and phase angle rate of change, in a fourstage sequence:

{[Sr(w) to the power of 2]*[Pa(z) to the power of 4]}=+wP, andconversely,

{[Sr(z) to the power of 2]/[Pa(w) to the power of 4]}=−zAP,

{[Sr(z) to the power of 2]*[Pa(w) to the power of 4]}=+zAP

{[Pa(w) to the power of 2]/[Sr(z) to the power of 4]}=−wP.

Then, if you postulate that:

[(+wP)+(−zAP)]=[(+zAP)+(−wP0}

then: +wP=[(+zAP)+(−wP)]/(−zAP)

Therefore: if you change either spin rate or phase of any of the abovecomponents, you change the status quo or dynamic balance of thesub-atomic particles and take charge of the resultant +wP. (nuclearweight of the proton=dimensional weight of the photon).

Therefore: {[Sr(w) to the power of 2]*[Pa(z) to the power of 4]}=hDW(Holographic Dimensional Weight) or mass of sub-atomic particles theelectron of atomic structure, i.e. visual data to the brain via the rodsand cones of the scanning system of the human eyes, dimensionality,(phase rate or dimensional weight) can be controlled.

By holographing the phase structure of electrons, we then take controlof the phase angle of sub-atomic particles. By resetting the spin rateand change of phase rate of sub-atomic particles, we then controldimensional weight, (i.e., we then can control dimensional imagery,produced as a sub-atomic electron hologram.)

What is shown is a mechanism that holographically phases sub-atomicparticles to emulate and even replicate the true dimension of real lifeas interpreted by control structure of human eyesight, by a method andelectronic apparatus mechanism that holographically phases thesub-atomic structure of atomic mass to change atomic structure orcontrol of the holographic spin rate of photons which is interpreted bythe human sight systems a replication of real life dimensional imagery.

By phased focusing of the beams of the electron guns of a CRT toward theobject pixels, red, green and blue dots of the CRT, the energeticelectron beams of the CRT being sub-atomically phased, you can thenchange the pixel dot sub-atomically phased into a bibble of the objectimagery being illuminated, causing a real life like or dimensionalsystem of imagery, or true life replication, by means of holographicelectron imagery displayed on a television screen.

Whether of photons or atoms, etc., rate of spin determines thedimensional weight and phase of the mass of the object. i.e. gravityintensity of the core or nuclei Sr(x)=[G(x)2]when G=[Sr(prp)2]. Evenphotons have mass and spin rates with an electron vacuum core withresulting vertical poles.

By changing the photon phasing, the resulting poles are realigned. Withsub-atomic replication, or phasings, you can have a new kind of imagery.(i.e., Simply by changing a photon group bibble (bibble refers to groupphasing of a cluster of photons which are organized into 6 differentdistinct phased phasings, organized similarly to bits, and bytes of acomputer system. One pixel of a television screen is mutedconstructively and destructively by the hologram phasing into multipledistinctive phasings.)) Phased sub-atomic particles hologram a newholographic version of the old two-dimensional imagery which isreplicated to the CRT as a visual hologram.

Holograms are known and visualized in nature, such as rainbows, layeredfrost on a window, or they can be produced with split laser beams ofcoherent light; or magnetically produced as seismographical equipment,or as in our description, they can be produced by sub-atomic patternsphased against each other to produce holographic visual scenes,coherently.

Sub-Atomic-Mueon phasing is the heart of this invention, and presents anew form of holography as related to visual replication, indeed a newform of controlling and manipulating visual imagery, electronically.

By holographing the phase structure of electrons, we then take controlof the phase angle of sub-atomic photon particles. By resetting the spinrate and phase of sub-atomic particles, we then control thedimensionality phase.

By controlling the spin rate and phase rate, dimensional weight [Sr(x)2Pr(x)4] of sub-atomic particles the electron mass of photons arerestructured into a high density dimensional holographic visual scenedisplayed on a standard CRT.

In FIG. 11, is shown a high density dimensional regenerative sub-atomicmueon phaser control circuit. It is an improved method, to control thephasing of the PLLs of FIG. 12, with which to spin phase the mutingsub-atomic mueon encoding of FIG. 13. It is so named because it spinphases the two main control pulses 7A and 8B conversely, and alternatelyphases them [(Z/K)*(n+y) to the exponential power xa] and [(Z/K)*(n−y)to the exponential power xa] degrees behind each other and spins themsimultaneously in opposite rotation to each other in a phasedconfiguration.

This is accomplished by the combination of two programmable up-down 0-3counters 5 and 6. Four digital thumbwheel switches #11R, 12S, 13U and14V, are arranged is such a manner that their presets alternatelyprogram successively the input jams of counters 5 and 6 to produceabcdefgh digital counts, which are fed to the to the program abcdefghinputs of the 7D and 8D counters. These counters are clocked at 7C and8C by external control signals which are fed back from down stream inthe signal generating process, (the “A” 72 output of FIG. 12 tied to the“B” 8C input of this circuit and conversely, the “B” 73 output of FIG.12 tied to the “A” 7C input of this circuit) giving crossover x-powerexponential regenerative holographic variable control frequencies forthe proper ultimate sub-atomic mueon muting for destructive andconstructive holographic sub-atomic mueon phasing control injectionsignals.

The outputs of the digital thumbwheel switches #11R, 12S, 13U and 14V,are fed to the abcdefgh program inputs of counter #5 which programs itto a count always exactly [(Z/K)*(n+y) to the exponential power xa] and[(Z/K)*(n−y) to the exponential power xa] degrees out of phase with theother counter #6. (This causes the counters 5 and 6, to always count inopposite directions to each other in a precise four phased manner, byfinal means of the routing bus multiplexer 17, which alternatelyexchanges the control presets 13 and 14 with thumbwheel control presets11R and 12S.)

The sub-atomic mueon phaser's program counters 5 and 6 are clocked atinput #16.

The Vertical Drive Clock pulses #16 are routed via multiplexer 2 toeither inverter #3 or #4 which alternately clock the up down gates forthe up and down clocking of program counters #5 and #6, as determined bythe said 1-2 multiplexer #2 which with the help of inverters 3 and 4,and analog switches 3A and 4B, changes the source of preset count ofdigital thumbwheel switches set #11R and 13U, or set 12S and 14V, ascounters 5 and 6 reach 0, either up or down, from their respective ncount. This causes the input presets of the counters #5 and #6 to resetup and down consecutively and always in opposite direction from eachother, for phases 1 and 2, then exchange sets of presets between set 11Rand 13U, or set 12S and 14V preset jam numbers.

Flip-flop #1 simultaneously changes the up/down phasing count of theoutput of counters #6 and #5, causing them to alternately lead or lageach other [(Z/K)*(n+y) to the power of xa]−[(W*K)/(n−y) to the power ofxb] degrees out of phase with each other in a precise manner, byclocking the up/down inputs of the counters 5 and 6. Every time thecounters complete an up/down or down/up cycle, their reset pulse clocksa shared “OR” gate 9, which clocks flip-flop 1 to change direction ofthe up/down busses 4B and 3B. The Q′ outputs of flip-flop 1 clocksflip-flop 10 which exchanges the buss outputs of buss routingmultiplexer 17. This gives the sub-atomic mueon phaser a four cyclephasing pattern. Digital outputs #7 and #8 presets the programmablecounter 7D and 8D, whose “A” and “B” outputs preset in turn, thecounters #10 and #9 of FIG. 12 of the dual holographic 4 phase spinningcontrol digital encoding PLLs of FIG. 12; which clock phases and spinsthe sub-atomic mueon encoded “A” and “B” n1, n2, . . . n8 degree mutingcontrol signals of the final holographic muting encoding control signalsof FIG. 13 which are injected into the television envelope (21-26 ofFIG. 13) to produce the holographic visual scene as generated on atelevision screen or monitor, via in and out composite video connections27 and 28 of FIG. 13.

In FIG. 12 where the “X” phaser (#3) and the “A” and “B” programmablephase lock loop #2 and master programmable divider #1 are shown, is theorigin of the two, “X” two phased control signals, namely the“A”+/−signal Sub-Atomic-Mueon control phasing

[(Z/k)*(n+y) to the exponential power xa]

and [(Z/k)*(n−y) to the exponential power xa]

developing alternate phased constructive exponentially curved forcelines, and the +/−“B” control signals

[(W*k)/(n−y) to the exponential power of xb]

and [(W*k)/(n+y) to the exponential power of xb]

developing alternate phased destructive Sub-Atomic-Mueon straight linecontrol Phasings. These two converse signals, “A” and “B”, spinning inforward and reverse rotation, forming dual control, four phased signalpulses #61 and #60, are the building blocks of proton and anti-protonsimulation of the W and Z energetic electron mueon control of theelectro weak force which electronically encode the dual Sub-Atomic-Mueonstrong force phased control system signals, which in turn control theelectrons of the electro-magnetic strong force.

Looking again now at FIG. 12, the television subcarrier sync signal (#4)is divided by “k” (the proton nucleus atomic weight multiplier, set at90 to match the Cern experiment, set by thumbwheel switch 74D) via ncounter #74 and fed to via input #2A to master X PLL, to develop theconstructive “A” holographic signals. The 4.5 MHz audio carrier signalinputted at (#4B) is routed to pre-scalar multiplier PLL (#74B) whoseoutput “K” factor is set at 80, by thumbwheel digital switch 74C, tomatch the Cern anti-proton weight factor, and inputted to master divider“B” to develop the alternate respective destructive control frequencies.The television system vertical drive sync pulse, (4A) clocks the “X”Phaser, via its input #16.

The most (#9 and #10) significant bits (m−1) of the programmable presetinputs of the divider counter of PLL loop #11 and master divider counter#12 of programmable phase lock loop “A” and master divider “B” #1 and #2are programmed or switched by the “X” phaser A and B outputs (#7A and#8B of FIG. 12).

Thumbwheel switch #13A and 13B post scales the final range andreciprocal feedback ratio of the output of the master phase lock loopand master divider, to the nominal one to six megahertz range of thefinal outputs of FIG. 13 for the NTSC television band width range. (Thisrange set with regard to the final output ranges of desirablecompatibility of the system being processed; namely NTSC, PAL, SECAM orHigh Definition applications, of which the latter may go up to rangesincluding 20 to 30 MHz.)

Analog to digital converter #7 of FIG. 12 converts the fundamentalsystem control signal #58, to the abed (first four) significant bits ofthe PLLs “A” divider feedback loop #11 (16 bit configuration).

Analog to digital converter #8 of FIG. 12 converts the fundamentalsystem control signal #59, to the abcd (first four) significant bits ofthe PLL's “B” master divider counter #12 (16 bit configuration).

In accordance with the inventors' discovery that the brain sees andhears holographically on a relative reciprocal basis, D/A converters #7and #8 are cross encoded by inserting the same abcd preset controlbusses to the next four significant bits of the “A” and “B” master phaselock loop and master divider's opposite side (i.e., the “A” or #7 A/Doutput is also routed to the “B” efgh section of the presets of themaster divider “B”.) Conversely the “B” or #8 A/D output is also routedto the “A” efgh section of the presets of the master phase lock loopdivider “A” of the audio and video signals respectively at #58 and #59,to complete a multiple reactive feedback path to encode the brainholographically by the alternate cross feedback perception paths (7A and8B). The final “A” and “B” control pulses are exited at outputs #72 and#73. The control signals to the Sub-Atomic-Mueon switching section ofthe circuit are outputted in four distinct phases and configurations:

Phase 1:

“A” is rotating clockwise ascending (from count presets 11R and 13U ofFIG. 11) varying by Sub-Atomic-Mueon constructive and destructivefeedback means of the A/D converters #7 and 8 of FIG. 2) and destructiveexponential feedback signal 8D.

“B” is rotating counterclockwise descending (from count presets 12S and14V of FIG. 11) the said count varying by Sub-Atomic-Mueon destructiveand constructive feedback means of the A/D converters #7 and #8 of FIG.12 and constructive exponential feedback signal 7D.

“A” leads “B” by {[(Z/k)*(n+y) to the power of xa]−[(W*k)/(n−y) to thepower of xb] degrees. [Where z is the frequency of the systemsub-carrier (4 of FIG. 12), where W is the frequency of the system audiocarrier (4B of FIG. 12), k is the prescalar divider (74 of FIG. 12 andn=the preset inputs (11R and 13U of FIG. 1) and y is defined as theclock input pulses (16 of FIG. 11), and xa and xb being defined by theabove said feedback means (#7D and #8D of FIG. 12)]

Phase 2:

“B” is rotating clockwise ascending (from count presets 11R and 13U ofFIG. 11) varying by Sub-Atomic-Mueon constructive and destructivefeedback means of the A/D converters #7 and 8 of FIG. 12 andconstructive exponential feedback signal 7D.

“A” is rotating counter clockwise descending (from count presets 12S and14V of FIG. 11) varying by Sub-Atomic-Mueon destructive and constructivefeedback means of the A/D converters #7 and #8 of FIG. 2 and destructiveexponential feedback signal 8D.

“B” leads “A” by {[(W/k)*(n−y) to the power of xa]−[(Z*k)/(n+y) to thepower of xb] degrees. [Where z is the frequency of the systemsub-carrier (4 of FIG. 12), where W is the frequency of the system audiocarrier (4B of FIG. 12), k is the prescalar divider (74 of FIG. 12) andn=the preset inputs (11R and 13U of FIG. 11) and y is defined as theclock input pulses (16 of FIG. 11), and xa and xb being defined by theabove said feedback means (#7D and #8D of FIG. 12)]

Phase 3:

“A” is rotating clockwise ascending (from count presets 12S and 14V ofFIG. 11 varying by Sub-Atomic-Mueon constructive and destructivefeedback means of the A/D converters #7 and 8 of FIG. 12) anddestructive exponential feedback signal 8D.

“B” is rotating counter clockwise descending (from count presets 12S and14V of FIG. 11) varying by Sub-Atomic-Mueon destructive and constructivefeedback means of the A/D converters #7 and #8 of FIG. 12 andconstructive exponential feedback signal 7D.

“A” leads “B” by [[(W/k)*(n+y) to the power of xa]−[(Z*k)/(n−y) to thepower of xb]} degrees. [Where z is the frequency of the systemsub-carrier (4 of FIG. 12), where W is the frequency of the system audiocarrier (4B of FIG. 12), k is the prescalar divider (74 of FIG. 12) andn=the preset inputs (12S and 14V of FIG. 11) and y is defined as theclock input pulses (16 of FIG. 11), and xa and xb being defined by theabove said feedback means (#7D and #8D of FIG. 12)]

Phase 4:

“B” is rotating clockwise ascending (from count presets 12S and 14V ofFIG. 1) varying by Sub-Atomic-Mueon constructive and destructivefeedback means of the A/D converters #7 and #8 of FIG. 12 andconstructive exponential feedback signal 7D.

“A” is rotating counter clockwise descending (from count presets 11R and13U of FIG. 11) varying by Sub-Atomic-Mueon destructive and constructivefeedback means of the A/D converters #7 and #8 of FIG. 12 anddestructive exponential feedback signal 8D.

“B” leads “A” by {[(W/k)*(n−y) to the power of xa]−[(Z*k)/(n+y) to thepower of xb] degrees. [Where Za is the frequency of the systemsub-carrier (4 of FIG. 12), where Zb is the frequency of the systemaudio carrier (4B of FIG. 12), k is the prescalar divider (74 of FIG.12) and n=the preset inputs (12S and 14V of FIG. 1) and y is defined asthe clock input pulses (16 of FIG. 11), and xa and xb being defined bythe above said feedback means (#7D and #8D of FIG. 12)]

In FIG. 13 is shown the final implementation of the Sub-Atomic-Mueonencoded muting holographic process. It is dependent upon the “A” and “B”“X” phaser control pulses from #72 and #73 of FIG. 3.

In FIG. 13: Two 45 degree generators n1 and n2 . . . to n8 degrees, (1and 2) n1 being 45 degrees, n2 being 90 degrees, n3 being 135 degrees,etc. These said phase generators being clocked respectively by the “A”and “B” Sub-Atomic-Mueon control signals generated by circuitry of FIG.12 outputted at 72 and 73 of FIG. 12.

Sub-Atomic-Mueon muting (via analog switches 15, 16, 18 and 20) of theinjected sideband control sub-subcarriers (10 and 14) and (11 and 13)are dual phase encoded directly with Sub-Atomic-Mueon phasing (buss “A”and “B” X phased 34 and 35) via intermediary PLLs (1C, 1D, 2C and 2D)specially referenced exponentially, by the means of special musical notecontrol (via special audio generators 36, 37, 38 and 39) frequencies,whose harmonic relation to each other produces the spatial holographicmodel muting, (via analog switches 15, 16, 18 and 20) that when injected(via inductance capacitance means 21, 22, 25 and 26) into the final NTSCor PAL, or SECAM television signal envelope, dimensionalizes the finalvideo and audio imagery (via input 27 and output 28). The melodic scaleis Sub-Atomic-Mueon aligned with the universal melody of matter. (i.e.,the melodic scale which has experimentally fallen in line with greatmusical compositions of the ages is merely a reflection of the harmonyof the universe, which gives us phasing alignment for theSub-Atomic-Mueon hologram that matches biological systems of humanvisual sight and hearing.)

Four analog switches mute the four above described control frequenciesaccording to control pulses generated by the “two” “A” and “B” clockingcounters (#1 and #2 of FIG. 13) producing Sub-Atomic-Mueon phasedoverlapping selected phase n1, n2 . . . n8, (only two of the eight 45degree phases are utilized in this description, additional stages may becascaded as shown by dotted lines 1C, 1E, 16 a and 23) 45 degree pulseswhose outputs are exponentially expanded by programmable Phase LockLoops 1C, 1D, 2C and 2D. (Similar to the #1 PLL of FIG. 12, only with 8bit feedback dividers instead of 16 bit dividers) The 1st foursignificant bits of the internal programmable feedback loop dividers ofthese PLL and master divider are buss controlled manually by digitalthumbwheel switches #4A, 4B, 4C and 4D. (These individual controllersposition individually the phase position of the below described sidebandcontrol sub-subcarrier signals, for various applications and can be putunder external control manually or by computer. These thumbwheelexternal controllers can also be buss connected by thumbwheel switch 4,via buss connectors 5A, 5B and 5C.) The least significant bits of the“A′ side PLLs 1C, 1D are under control of the digital four bit output Aof the “X” phasor (#7A of FIG. 11). The least significant bits of the“B” side PLLs 2C, 2D, are under control of the digital most significantfour bit output B of the “X” Phasor (37 of FIG. 11). The buss thumbwheelswitches (4) control the most significant four input jams of thecounters of PLLs 1C, 1D, 2C and 2D. These PLLs control the dimensionalpositioning of the imagery. (The buss control can be connected at plug#5 to Cad Cam computers or video game controls for dimensionalpositioning under external computer control.) The outputs of the abovePLLs clock the gates of the analog switches (15, 16, 18 and 20).

Still looking at FIG. 13, the Sub-Atomic-Mueon signal phase encoders “A”(#1) and “B” (#2) mute the two sets of sideband control sub-subcarrierfrequency clocks. These clocks re derived by phase lock loop clockgenerators 11, 13, 10 and 14. These Sideband Control Sub-subcarriers aregenerated by formulas Cf*(T/Np,q,r,u,v or w) and Cf*(S/Np,q,r,u,v or w)where T or S is designated the prescalar for the said PLLs, C frequency(in this case v.s.c. the television system sub-carrier 3.58 MHz syncsignal is inputted at 4 of FIG. 12, and a.s.c. 4.5 MHz is inputted at 4Bof FIG. 12), and N is the division number of the divider feedback of thephase lock loop feedback system and N is a whole integer where S=80 orT=90. ((i.e., if t is designated 90 then, p=86, q=87, r=88, s=89, t=90,u=91, v=92, w=93, and if S is designated to be 80 then, p=77, q=78,r=79, s=80, t=81, u=82, v=83, w=84.) The scope of this invention is notlimited to the selection or example of the #90 as in this description tothe 45 degree phasing exampled here with 8 whole integers. ((i.e., t ors could be “26” instead of 90 with 60 degree phasing utilizing 6 wholenumber integers, or any convenient system of degree phasing andresulting group of whole # integers.) However the formula is valid aslong as the phasing is correlated to 90 times the nuclear weight of theproton and the opposite phase is correlated to 80 times the atomicweight of the anti-proton as in the W and Z discovery by the Cernexperiment referenced earlier.

The inventors have devised the following Sub-Atomic-Mueon proton nucleusatomic weight master ratio control, consecutive integer factor chart:

Proton “A” side PLL Constructive Interference 86 87 88 89 90 91 92 93exponential P Q R S T U V W curved line 2nd 1st intervals 3^(rd) 4thintervals P Q R S T U V W straight line 77 78 79 80 81 82 84 85 straightline Destructive Interference Anti-Proton “B” side Divider Counter 4th3rd 2^(nd) 1st intervals 1 2 3 4 1 2 3 1 2 * * * c c# d d# e f f# g g# aa# b c * * * * * * * * * 2 1 1 2nd 1st

The #11 sideband control sub-subcarrier frequency is formula generatedby a phase lock loop which is prescaled by dividing the televisionsystem subcarrier sync Cf (4 of FIG. 12) by T (90 in this case, inreference to the Cern experiments) and referenced to the said PLL, whichin turn multiplies the said reference input by its divide feedback loopwhose counter is set at two integer numbers below “T”, which is “Nr” or88 in this case.

The #13 sideband control sub-subcarrier frequency is formula generatedby a phase lock loop which is prescaled by dividing the master systemcontrol television system subcarrier sync frequency s.c. sync (4 of FIG.12) by T, (90 in this case) and referenced to the said PLL, which inturn multiplies the said reference input by its divide feedback loopwhose counter is set at the next integer number above T, “Nu” (91 inthis case).

The #10 sideband sub-subcarrier frequency is formula generated by aphase lock loop which is prescaled by dividing the television audiocarrier frequency, 4.5 MHz, (4B of FIG. 12) by S, (80 in this case) andreferenced to the said master divider counter (12 of FIG. 12), which inturn divides the said reference input by “Nw” (84 in this case).

The #14 sideband control sub-subcarrier frequency is formula generatedby a phase lock loop which is prescaled by dividing the television audiocarrier frequency, 4.5 MHz Cf (4B of FIG. 12) by 1 (80 in this case) andreferenced to the said PLL, which in turn multiplies the said referenceinput by its divide feedback loop whose counter is set at “Np” (77 inthis case).

In the NTSC version, the dual “video” sideband control sub-subcarrierclocks scCP(T/Nr) and scCP(T/Nu) #11 and #13 are analog switch muted byanalog switches #15 and #16. The “audio” dual sideband controlsub-subcarriers (T/Nr) and Cf*(T/Nu) clocks #10 and #14 are analogswitch muted by analog switches #18 and #20 respectively.

These holographically muted or switching sideband control sub-subcarrierpulses are then injected into the NTSC, PAL or SECAM envelope bycapacitance inductance coils, (#21, 22 25 and 26) which are capacitanceresistance tunable for proper inductance.

The composite video signal is inputted at input #27 and exited at output#28, as a fully dimensionalized holographic signal which will play outon any standard NTSC, PAL or SECAM receiver. The original compositevideo signals must be processed by subcarriers matching the particularsystem NTSC, PAL or SECAM; the sub-subcarrier clock frequencies of thisembodiment were selected for NTSC, however, the scope of this inventionis not to be limited to any one particular system of televisionbroadcasting format, only the controlling subcarriers of the particularsystem utilized, conformed to the particular subcarrier systems utilizedby the system. The result is a fully dimensional high definition imagesignal generated holographically on a standard television receiver ormonitor which can be recorded, or broadcast by standard means tosatellite or cable systems for viewing a three dimensional holographicimage on standard television receivers, monitors, or any CRT viewingsystem or computer CAD CAM systems, CAT SCAN systems or electronmicroscopic or telescopic systems.

FIG. 8 Section B

Looking now at the high speed muting section in FIGS. 8-1 to 8-3(Section B), is seen the dual set of RGB color video amplifiers VL1 andVL2 which bring the two sets of red, green and blue video signals, fromthe left and right CCD color pickups CD1 and CD2 of Axes A2 and A3, upto proper switching and processing voltages. As primary and secondarylight beams stream in through angled pinioned P1 and P4 lenses L1 andL4, combining with light from axes A2 and A3 to the left and right CCDRGB pickups CD1 and CD2, they are switched at the slow speed of VerticalDrive V3 switching pulses of the primary and secondary flip flops FF1and FF2, however the high speed holographic muting section of FIGS. 8-1to 8-3 section B is driven by imported high speed Sub-Atomic Phasings ofFIG. 12 at inputs SA1 and SA2 respectively, from the “A” and “B” (72 and73 of FIG. 12) X Phaser holographic control outputs. The said CCD colorpickups CD1 and CD2 are synchronized by camera control sync buss CC3which delivers normal television sync signals Vertical Drive, HorizontalDrive, and Subcarrier raster control signals. Vertical Drive (60 Hz inthe case of NTSC, 50 Hz in the case of PAL and SECAM world wide systems)is clocked via lead V3 to clock flip flops FF1, FF2 and FF5. Flip flopsFF3 and FF4 are clocked by the respective Q′ and Q outputs of framecontrol flip flop FF5. This allows both sub-rasters of both RGBamplifiers VL1 and VL2 to transmit in a four phase, four field frame.Primary color video delays D1 and D2 are manually set by pot controlsDS1 and DS2 for Pseudo 3-D dimensionalization when the StarCam lenssystem is bypassed and conventional pre-filmed video is reprocessed forPseudo dimensionality.

Digital AND GATES A1, A2, A3 and A4 are utilized to pulse under phasedcontrol of the four phase raster control flip flops FF# and FF4, thehigh speed holovidic control muting signals SA1 and SA2 imported fromthe external programmable phase lock loop holographic “X” Phasedgenerator of FIG. 12. The high speed muting output control pulses of thefour said AND gates A1, A2, A3 and A4 pass alternately in a four phasedpattern, of linticular secondary and primary holographically invisibleinterference patterns which are generated by combining the outputs ofRGB busses LB3 and LB4 to produce on the face of the televisionreceiver, a holographic dimensional imagery of visual scenes when viewedon a conventional TV receiver, without the aid of coded viewing glasses.

Automatic Holographic Language Track Translation Method for Television,Film, Audio and Print

Looking now at FIG. 10: This invention also concerns the holographicapplication of multiple language real time automatic selective languagetrack translations for film, television and written applications.

The holographic application concerns the real time identification of ahost language 4, syllable by syllable phonics recognition 1 at ultravariable nx high speed applications of preestablished voice soundrecognition patterns which are identified and returned in translatedsegments in phased and synchronized time delayed numbered segments,which encode the new assembled language to the host track 4. Thesynchronized and processed numbered encoding segments can then in realphased time, by made selective to the recipient chosen language track 5.

The following conventions will be utilized:

1. A numbered IPL phonic sound encoded recognition voice pattern memorybank 1, will be created by digitally recording the IPL (an internationalphonic language sound bank) phonic voice sounds in high medium and lowmale and female versions.

2. The host language dictionary 4, word by word will be encoded intomemory with the identified numbered IPL phonic designations 4A.

3. The video and audio tracks will be selectively delayed 1 to 3 secondssynchronously by a running digitally synchronized 1 to 3 second timedelayed moving frame store.

4. The voice audio track will be routed to the holographicallyalternately variable sweeping high speed IPL phonics analyzer comparison2, encoding processors, which after the second verification, willcompare to ensure accuracy and then will encode to the synchronized timeencoded host sound track, a series of IPL encoded code number, 4A of theidentified IPL voice segments.

5. The host language track memory at appropriate synchronized locations4A, will receive the designated IPL numbered segments.

6. Each IPL syllable will be stored into the host track memory with atime position stamp 4B, (hour, minute, second and 1/100th of a secondwhich will become its position locator in the host track memory. Thesesyllables will be stored in word groups. The time stamp stack mayoverlap some syllables (in which case the volume of these overlaidsyllables will be faded under the beginning of the next syllable). Theword groups (in IPL designated hex numbers) will then be compared withthe host word dictionary memory to retrieve and identify a recognizedword 2A. The host dictionary will contain numbered words which willmatch numerically to the recipient dictionary 4A to 4B. Each numberedword, with its a, b, c, d, e, f, and g (in order of most frequent orpopular use) thesauruses complements, in both dictionaries will alsocontain the IPL syllable designators. The IPL word bytes containing theassigned IPL numbers of the host track will be compared with the hostdictionary IPL sequence codes to be identified and then assigned to theappropriate time stamp location 7A of the recipient language track.

7. A recipient IPL language bank 5, will house numbered digitallyrecorded IPL audio segments 5C, in Lo, Med, and Hi voice samples bothmale and female. A, B, and C will be male designators. D, E, and F willbe male designators for the Lo, Med, and Hi audio digital samples. Eachvoice sample will also have a 1-7 volume level indicator number. Eachvoice sample will have a 12 note half step octave voice range frequencyindicator, an expanded 3 octave sampling will allow for singingtranslations, in addition to the male, female Lo, Med and Hi rangeindicators. Additionally each voice sample will contain a voicing selectindicator. A voice picture sampling will capture timbre voicingselection to duplicate voice recognition characteristics to imitaterecognition contours of each new voice as introduced into the film oraudio recording.

Individual voice recognition of the original host voice willautomatically be analyzed and imitated by the IPL sound byte samplememory track as they are played back 7B, by the recipient track 7. Themaster IPL sound samples 5C, will be altered by envelope contouring(frequency, duration, sound level and timbre) to match the original hostsound sample as the new translation is matched up by the recipientsynchronized voice sync sound track.

Once the host track has been processed and the IPL segments analyzed,grouped into word bytes, identified by the host IPL dictionary, andassigned a dictionary word number along with its appropriate voicingselect indicators, it becomes a master host track that can then beeither played back in real time as the processing occurs or be retainedin memory as a master track to be played out against any recipientlanguage track chosen for any selected language.

Each recipient language dictionary (French, German, Italian, . . . etc.)will have its words assigned the same identifier numbers withcorresponding words of the host dictionary, with each word of the samemeaning and grammatical designation (i.e., verb, gender, noun, adverb,location, data\HLANGTK7 . . . etc.) having the same identifying number,and a word byte of appropriate IPL numbers to facilitate automaticreplication of the time recipient track language word to be reproducedby the recipient track 7.

In the case of television replication by satellite, terrestrial cable,DBS or cassette tape, an early line scan can be assigned to recite andcontain the IPL word byte with its accompanying voicing indicators, aspositioned by the time stamp locator. Then language can be selected byan on site (black box on the television receiver) and the selectedlanguages be played out automatically as the signal is received. Theblack box would have in its internal memory the appropriate mechanism toplay out the IPL code with its accompanying voicing indicators as theinstructions are deciphered by the black box. The black box would beloaded by a plug in carriage 7B containing the desired recipientlanguage, with each word responding to the international language wordnumber code, and grammarians arranger, and automatically assigning thecorrect IPL phonics to be played out as word bytes in the new recipientlanguage. The black box could be loaded with several languagedictionaries to offer, a selection of languages at the flip of a dial.

In the production of material or programming to be utilized with theautomatic language track system or device, the voice track preferablyshould be recorded on a separate track from all other sound effecttracks. The black box will then mix in the new language to the soundeffects track. This procedure is inherently a cleaner reproduction ofthe translated track. Otherwise an alternate method of mixing will beassigned as follows:

1. The audio range of voicing will be filtered out to the recognitionholographic circuits 2.

2. In the recipient language track reproduction either in real time orauto language tracking reproduction the original voices (as Karaoke singalong methods) will be suppressed by appropriate audio filtering.

3. The recipient IPL language will be mixed over the original filteredsound tracks sufficiently loud enough to be heard and enjoyed by thelistener 7B.

The IPL designation word byte 5D, along with its voicing indicators willalso contain a holographic stereo sound positioning code for originalroom positioning of the played back voice track sound. (This code willindicate appropriate holographic information to position the sound as itwas originally recorded.)

Also, as an additional embodiment of this invention, the print mythologyor embodiment of this invention will embrace the following variations ofthis invention:

1. After the IPL holographic scanning of the voice track or recording ofvoice reading, and the IPL word bytes have been assigned to the hosttrack, (or for that matter, from any processed track of thismethodology) the international host dictionary numbers will be assignedto a word processing procedures connected to a computer word processor8A for typing in either host language or taken a step further andprocessed after the selected recipient language numbers 8B have beenassigned for automatic foreign language translation for printing only.This process may be used for automatic typing of voice dictation intoany language either one at a time as selected or into multiple languagessimultaneously, with multiple word processing computers systemsconnected to separate black boxes assigned to its selected recipientlanguage.

In the case of multiple language audiences, black boxes may bemultiplexed for any number of languages for selected separate languagerouting to appropriate earphones in the auditorium.

In the case of satellite transmission or tape distribution, black boxescan be utilized with plug in cartridges for the specific languages.

In the case of translations directly from a computer's word processor,the computers may be connected to the black box to directly translatefrom the word processor skipping the high speed holographic analyzingprocess and going directly to the IPL comparison state to translate thetext.

Also included within the scope of this invention, is a high speed meansof transmission of the holographic data utilized by this technology.

In FIGS. 14A and 14B is described a reactively programmable digitaldelay which also injects a programmable dual echo feedback loop whichtotally eliminates all microphone feedback and has multiple addressabledual access reader capability, which can exit a mono or stereoholographic dual output generated from one audio component.

The delay utilizes a 32 byte (bit byte 4096 register ram #1 which iscontinually written into by the output of a 12 bit analog to digitalconverter #8 which accepts the audio input #29 after it has beenbuffered by variable (volume) buffer #36. The said A/D output writesinto the ram #1 by direction of write address counter #45, via buss #46.The write address counter #45 is clocked by sample clock input #29.(This sample clock is twice the frequency of the band pass width of theaudio component being delayed; however this clock is divided by thenumber of bytes selected to be utilized as programmed by thumbwheeldigital switch #31, to give more time for the appropriate number ofbytes to be additionally entered into the particular register which thecounter pointer digital buss #46 is indicating.) In each of the 4096registers of the ram #1 one to thirty two bytes are written in asprogrammed by register size counter #4 which is controlled by digitalthumbwheel register size switch #31, (this multiplies the capacity ofthe ram #1 to adjust for the frequency limits of the bandpass beingprocessed; Hi frequencies take more memory space in the ram 0). Beforethe next register is accessed by the write address counter #45.

For Lo Band Pass applications the master sampling frequency is 600 cps.The Dual Access Delay will produce a 1.666 milli-second delay for eachincrement or register number set by thumbwheel switch # was set at 2bytes per register.

For Mid Band Pass applications the master sampling frequency is 6000cps. The Dual Access Delay will produce a 0.1666 milli-second delay foreach increment or register number set by thumbwheel switch 18A or 18B. Asetting of 1000 would produce a 1.333 second delay if the register sizethumbwheel switch #31 was set at 8 bytes per register.

For Hi Band Pass application the master sampling frequency is 60000 cps.The Dual Access Delay will produce a 0.01666 milli-second delay for eachincrement or register number set by thumbwheel switch 18A or 18B. Asetting of 1000 would produce a 0.466 second delay if the register sizethumbwheel switch #31 were set at 28 bytes per register.

The delay has three sampling speed clock; the main reference clock isimputed at #3 and clocks the master analog to digital converter 8; theother two secondary sampling clocks are plus and minus 1% of the speedof the master sampling clock input #3. This makes the delay moredimensional and stops feedback distortion.

The Lead Read Counter #2A and Lag Read Counter #2B alternatelyconcurrently exchange the use of the two 99% and 101% sample clockpulses from input #52 and #64. The two sampling clock pulses are fed to2 to 1 multipliers #66 and #68, which are under the clock control, flipflops are clocked by theory outputs of counters #2A and 2B andalternately of counter #49.

The Q outputs of the above said flip flops #65 and #10 alternatelyenables and dis-enables the programmable function for the programmablelead and lag read address counters 2A and 2B. As these flip flops arealternately clocked by either their carry output of the respective readaddress counter or the carry output of counter #49, the counter #2A and2B are allowed to “wrap around” for a complete count cycle. (Fromprogrammed start through the zero count on upward again until the nextalternate reset which reprograms a new start number in the particularcounter 2A or 2B. Optical buffers #62 and #63 isolate the two counters#2A and #2B.

The use of the above stated plus and minus sampling clocks accomplishestwo objectives: first, external distortion feedback is completelyeliminated from the audio circuit; secondly, the special relation of thesound of the two outputs generated by the delay, are exponentiallydelayed to create a spatial relationship which creates dimensionally byexponentially expanding the delay slightly apart and inwardly(alternately a longer and shorter delays created in a pulsatingfashion).

The above stated variable delay is further enhanced under control ofmulti programmable clock inputs of the above stated lead and lag addresscounters #2A and #2B. The programmable inputs are divided into 3 inputnumber bytes of four bits each; a least significant byte, a middle byte,and a most significant byte. (This is in the program jam inputs of thecounters #2A and #2B, each one being a string of three cascaded 74193TTL counters, one for each four bit byte.)

The most significant bits of the above said lead and lag counters #2Aand #2B, are programmed by output of digital thumbwheel switch #18 whichis buss connected to the jam inputs of the two counters, which programsthe two counters to read a certain number of registers behind the masterwrite counter and apart from each other to give a programmed delay. Thephase difference between the two read out counters is also enhanced bythe mid and least significant bytes of the said counters. The mid bytesbeing programmed by the left and right outputs (#6 and #7 of FIG. 16) ofthe “L” phaser of FIG. 14B, via inputs 9A and 9B.

The least significant bits to the programmable jam inputs of the saidcounters #2A and #2B are programmed by outputs of four bit analog todigital converters #11 and #12. These A/D converters read the outputsignals of audio frequency comparators #13C and #59. These comparatorsproduce a voltage output reactive to the frequency of its input versusthe frequency of the sampling clocks imputed to give a reactive quotientoutput relative to the two frequencies. Based on a discovery by theinventors that, the higher the frequency of count the faster it travels;thus effecting echo and reverberation with respect to frequency andvolume, making higher pitches have less reverb time. Thus an assumptionwas made that additional or less delay should be programmed by afunction of frequency. To accomplish this, the output busses #25 and #24are digitally inverted by byte wide inverters #24A and #25A. So we noware programming the lead and lag read counters #2A and #2B to beresponsive to manual setting by digital thumbwheel switches 18A and 18Bto program the basic delay from the master register counter in the mostsignificant bytes, holographic “L” phasing in the mid-bytes, and anadditional small delay which a reverse function of frequency in theleast significant bytes; with the difference between digital switches#18A and #18B, determining the primary lag between the lead and lag read#2A and #2B, which is additionally variable by the extent of theprogramming of the mid and least significant bytes, to determine thespatial relationship of the final audio outputs #38 and #41 to eachother.

The multiple addressable dual readout ram has 4096 registers organizedinto 32 12 bit bytes per register. These registers are accessed almostsimultaneously, as enabled by a tri phased generator which is clocked bythe master sample clock (#2A of FIG. 15) and inputted at input #3. The0, 120 and 240 degree outputs of this tri-phased generator #51 areconnected to the master write, lead read and lag read enable inputs ofthe said multiple access ram #1. The leading edge of these phased pulsesenables the timing of the write and two read functions. The 120 degreephase output clocks the master numerical word byte write function, frommaster analog to digital converter #8. Tri-phased generator #51 directstraffic for the master input buss #8A, and the two read and lag outputbusses #16 and #15. The 120 degree phase pulse output clocks the masterwrite byte into the ram at the address pointed to by the write addresscounter #45 and the byte counter #4. The 240 degree phase pulse enablesthe lead read function, to read out the byte onto buss #29 which thelead read counter and byte counter pointers are indicating. The 0 degreephase pulse enables the lag read function, to read out the byte ontobuss #29 which the lag read counter and byte counter pointers areindicating.

The Lead Read Digital to Analog converter #42 is clocked by the outputof two to one multiplexer #65 which alternately feeds either the 99 or101 percent sampling clocks imputed at #62 and #64. (The sampling clockgenerators are shown in FIG. 15) Its analog output is buffered byvariable optical buffer #37 whose output is fed back to the input of themaster write analog to digital converter #8 to introduce a measuredamount of delayed echo from the 1st outputted audio channel line #38.

The Lag Read Digital to Analog converter #39 is clocked by the output oftwo to one multiplexer #65 which alternately feeds either the 99 or 101percent sampling clocks imputed at #62 and #64. (The sampling clockgenerators are shown in FIG. 15) Its analog output is buffered byvariable optical buffer #40 and fed back to the input of the masterwrite analog to digital converter #8 (after being optically bufferedagain by optical buffer #43 to keep the two audio channels #38 and #41isolated from each other) to introduce a measured amount of delayed echofrom the 2nd outputted audio channel line #38. The result is spatiallydimensional dual echo delayed reverberation which is holographic innature because of the buffered interference patterns of the audio as itis remixed by optical buffer #37 and #43 and fed back into the audioenvelope before it is redigitized by master A/D converter #8. Either ofthe lead or lag digital outputs #47 and #50 or the channel 1 and 2outputs #38 and #41 are spatially phased differently from each other andare dimensionally delayed at different phased delays and then bothcontain selected diminishing delayed echo portions of the lead and lagaudio channels, to give two audio channels for one original audiocomponent, which are spatially opposed to each other, each being acomplete holographic dimensional audio component within itself.

What is claimed is:
 1. A holographic muting lens camera systemcomprising: a dual axis four lens system operable to be angularlyadjusted to receive light along a first optical axis, a second opticalaxis, a third optical axis, and a fourth optical axis respectively; fourLCD switching elements operable to receiving light through the dual axisfour lens system; a pair of LCD switched dual filtered dichroic mirrorspositioned to receive light from the first optical axis and the fourthoptical axis; a pair of half silvered dichroic color filter elements forreceiving light along the second optical axis and the third optical axispositioned in an inverted v-shape at a 90 degree angle; and two chargecoupled device (CCD) pickups operable to receive light along the secondoptical axis and the third optical axis being spaced apart andsubstantially parallel, wherein the light from the second optical axisand the third optical axis is combined with light received along thefirst axis and fourth axis respectively through a plurality of halfsilvered mirrors for processing by the CCD pickups, wherein theplurality of half silvered mirrors are operable to reflect lightreceived through the first optical axis, the second optical axis, thethird optical axis, and the fourth optical axis reflected orcommunicated through the four LCD switching elements, the pair of LCDswitched dual filtered dichroic mirrors, and the pair of half silvereddichroic filter elements to produce optical disparity for dimension.